Early results of Agarwal and Jha [Z. Phys. B 35, 391 (1979)] are used to examine the question of quantum jumps in a Raman ({Λ}) system driven by two coherent fields. We discuss both short-time (γ₁t{}1) and long-time (γ₂t{}1) behavior of the intensity correlations assuming that the Stokes transition is very weak, γ₂{}γ₁. We calculate the counting statistics of the dark periods using the higher-order intensity correlations. The results differ from those obtained using arguments based on population trapping which predict only a very rare ``jump'' event. The intermittence in fluorescence produced by a coherently driven {Λ} system is interpreted in terms of an equivalent two-state Markov process.
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Agarwal et al. (1988) studied this question.
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